Enhanced thermoelectric performance of famatinite double-doped with Ge and Se

Famatinite (Cu 3 SbS 4 ) is a promising thermoelectric material with narrow bandgap. However, because its intrinsic carrier (hole) concentration is low, its electrical conductivity is low; thus, doping (partial substitution) is necessary to improve its thermoelectric performance. In this study, Cu 3...

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Veröffentlicht in:Journal of the Korean Physical Society 2024, Vol.84 (8), p.626-633
Hauptverfasser: Park, Sang Jun, Kim, Il-Ho
Format: Artikel
Sprache:eng
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Zusammenfassung:Famatinite (Cu 3 SbS 4 ) is a promising thermoelectric material with narrow bandgap. However, because its intrinsic carrier (hole) concentration is low, its electrical conductivity is low; thus, doping (partial substitution) is necessary to improve its thermoelectric performance. In this study, Cu 3 Sb 1– x Ge x S 4– y Se y ( x  = 0.04–0.06 and y  = 0.25–0.50) famatinite compounds double-doped with Ge and Se are prepared through solid-state synthesis. Phase analysis and microstructural observations are conducted, and the charge-transport characteristics and thermoelectric properties are examined according to the doping levels. All specimens contain a single phase of famatinite and behave similar to degenerate semiconductors. As the Ge and Se doping amounts increase, the electrical conductivity increases (6.99 × 10 3 –1.23 × 10 4 Sm −1 at 323 K) because of the increase in the carrier concentration (1.28 × 10 19 to 1.86 × 10 19  cm −3 ) In contrast, the Seebeck coefficient decreases from 211 to 168 μV K −1 at 323 K, exhibiting p-type conduction characteristics. The power factor is significantly increased by the double doping with Ge and Se, and Cu 3 Sb 0.96 Ge 0.04 S 3.50 Se 0.50 achieves a maximum power factor of 0.63 mW m −1  K −2 at 623 K. The thermal conductivity decreases with increasing temperature but increases with increasing doping amount. As a result, the dimensionless thermoelectric figure of merit ( ZT ) is improved by double doping with Ge and Se, especially at high temperatures, and a maximum ZT of 0.51 is achieved at 623 K for Cu 3 Sb 0.96 Ge 0.04 S 3.50 Se 0.50 .
ISSN:0374-4884
1976-8524
DOI:10.1007/s40042-024-01044-4